§ 1. Riesz spaces and fully lattice-ordered spaces
1. Definition of Riesz spaces
Recall that, on a set E, a vector space structure over the field and an order structure are said to be compatible if they satisfy the following two axioms:
(OVS_I) The relation implies for all .
(OVS_{II}) The relation implies for every scalar .
The space E, equipped with these two structures, is called an ordered vector space (TVS, II, §2, No. 5).
Axiom (OVS_I) signifies that the order structure and the additive group structure on E are compatible, in other words that E, equipped with these two structures, is an ordered group (A, VI, §1, No. 1).
Axiom (OVS_I) implies that the relations and are equivalent. Similarly, it follows from (OVS_{II}) that, for every scalar , the relations and are equivalent, because and so the relation implies . One can therefore say that, in an ordered vector space, the translations and the homotheties of ratio are automorphisms of the order structure; this fact is also expressed by saying that the order is invariant under every translation and every homothety of ratio . Moreover, the symmetry is an isomorphism of the order structure of E onto the opposite order structure.
Definition 1
An ordered vector space is said to be a Riesz space (or lattice-ordered vector space)* if its order structure is a lattice-ordering (that is, if every pair of elements of E has a supremum and an infimum ).
(1) Also called a "vector lattice".
(2) Borne supérieure (supremum) is also translated as "least upper bound" (S, R, §6, 7). Similarly borne inférieure (infimum) is also translated as "greatest lower bound".
Example
The space of all real-valued functions defined on any set is a Riesz space (for the order relation ); for, any two real-valued functions defined on have a supremum (resp. an infimum) equal to the mapping (resp. ).
One can also say that a Riesz space is a vector space equipped with an order structure such that, on the one hand, this structure and the additive group structure of define a lattice-ordered group structure on (A, VI, §1, No. 9), and on the other hand that the axiom (OVS) is satisfied.
Thus, all of the properties of lattice-ordered groups are applicable to Riesz spaces; we shall review here the principal ones (cf. A, VI, §1, Nos. 9 to 12), as well as indicating the consequences that flow from the axiom (OVS).
We recall first that one writes (the positive part of ), (the negative part of ), (the absolute value of ); then and ; here, these two relations are equivalent to
The relation is equivalent to . For any and , the triangle inequality holds:
(1)
By the invariance of order under every homothety of ratio ,
(2)
In particular,
(3)
On the other hand, for we have and ; it follows that, for every and every ,
(4)
The invariance of order under translation shows that for all ,
(5)
(6)
We have the relations
(7)
(8)
If are then (A, VI, §1, No. 12, Prop. 11)
(9)
If A and B are two subsets of E each of which has a supremum, then A + B also has a supremum and
(10)
Two elements of E are said to be alien (to each other) if ; by (8), this relation is equivalent to , and also, by (6), to ; 0 is the only element alien to itself; for every , and are alien and may be characterized as the only alien elements such that . If is alien to , then every such that is also alien to . If and are alien to , then so is , by the inequality (9); in particular, is alien to for every integer , from which it follows that is alien to for every scalar , since there exists an integer such that , whence . If a subset A of E consists of elements alien to and if A has a supremum, then that supremum is also alien to (A, VI, §1, No. 12, Cor. of Prop. 13).
Finally, we have the decomposition lemma (A, VI, §1, No. 10, Th. 1):
If* are two finite sequences of elements of E such that , then there exists a finite sequence of elements of E such that for all , and for all .
2. Generation of a Riesz space by its positive elements
Let E be an ordered vector space; the set P of elements of E is a convex cone with vertex 0, that is (TVS, II, §2, No. 4), a set such that
The original is étrangers, also translated as "coprime" (A, VI, §1, No. 12); the terms "orthogonal", "disjoint" and "mutually singular" are also used.
P + P ⊂ P and λP ⊂ P for all λ > 0. Conversely, if, in a vector space E over , P is a convex cone with vertex 0, such that (in other words, a pointed and proper convex cone), one knows (loc. cit.) that the relation is an order relation (denoted ) compatible with the vector space structure of E. For this order structure to define a Riesz space structure on E, it is necessary and sufficient that:
P generates E, that is, every is of the form , where x and y belong to P;
P satisfies one of the following two conditions: a) every pair of elements of P has a supremum in P; b) every pair of elements of P has an infimum in P (A, VI, §1, No. 9, Prop. 8).
3. Fully lattice-ordered spaces
Definition 2
A Riesz space E is said to be fully lattice-ordered if every nonempty subset of E that is bounded above has a supremum in E.
It is immediate that in a fully lattice-ordered space E, every nonempty subset that is bounded below has an infimum in E.
Example
— 1) If A is any set, the space of real-valued functions defined on A is fully lattice-ordered, the supremum in of a family that is bounded above being its upper envelope (GT, IV, §5, No. 5).
2) Let F be any set; the space of bounded real-valued functions on F, equipped with the order structure induced by that of , is fully lattice-ordered. However, if F is a topological space, the space of continuous real-valued functions on F (equipped with the order structure induced by that of ) is a Riesz space that is not in general fully lattice-ordered (cf. Exer. 13). Consider for example the case that ; let I be the interval ]0, 1[, the characteristic function of I, and let H be the set of continuous functions such that ; it is clear that H is bounded above in . The function is the upper envelope of the , but it is not their supremum in , since is lower semi-continuous but not continuous. Let us show that, in fact, H has no supremum in ; it suffices to prove that if is a continuous function such that , then there exists a continuous function such that . Now, , therefore there exists a number such that for ; if w is a continuous function that is zero outside of the interval ] and is such that on this interval, then the function meets the requirements.
Cites 1
Proposition 1
For an ordered vector space E to be fully lattice-ordered, it is necessary and sufficient that E be a Riesz space and that it satisfy one of the following two conditions:
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a) every nonempty subset A, consisting of elements of E, that is bounded above and directed for the relation , has a supremum in E;
b) every nonempty subset , consisting of elements of and directed for the relation , has an infimum in .
The conditions are obviously necessary. Conversely, suppose that is a Riesz space satisfying the condition a). Let be a nonempty subset of that is bounded above; the set consisting of the suprema of the finite subsets of is directed for the relation ; let be one its elements and the set of that are ; if we prove that has a supremum then it will also be the supremum of . Now, is a set of elements , bounded above and directed for the relation ; it therefore has a supremum , consequently is the supremum of .
On the other hand, the condition b) implies a): for, if is a nonempty set of elements of , bounded above and directed for , and if is an upper bound for , then is a set of elements that is directed for ; if it has an infimum , then is the supremum of .
Proposition 2
— Let be a Riesz space equipped with a Hausdorff topology that is compatible with its ordered vector space structure (TVS, II, §2, No. 7). If, for every set that is bounded above and directed for the relation , the section filter of is convergent, then is fully lattice-ordered.
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Indeed, one knows that the limit of the section filter of is the supremum of in (TVS, II, §2, No. 7, Prop. 18).
4. Subspaces and product spaces of fully lattice-ordered spaces
Let be a fully lattice-ordered space, a linear subspace of . The order structure induced on by that of is compatible with the vector space structure of , but the ordered vector space so defined is not necessarily a fully lattice-ordered space.
More precisely, it can happen that is not a Riesz space (Exer. 2), or that is a Riesz space but is not fully lattice-ordered: the latter is the case for the subspace of the space (No. 3, Example 2).
Moreover, if is a Riesz space (fully lattice-ordered or not) it can happen that the supremum in of two elements of is different from their supremum in (Exer. 3 b). Finally, it can happen that is fully lattice-ordered, that the supremum of each finite subset of is the same in and in , but that there exist infinite subsets of , bounded above in , for which the suprema in and are different (Exer. 13 f)).
Let be any family of ordered vector spaces. Recall that, in the product space , the product order relation of the order relations of the factor spaces is the relation (S, III, §1, No. 4). One verifies immediately that this relation is compatible with the vector space structure of E; E, equipped with this structure, is called the product space of the ordered spaces .
Proposition 3
Let be a family of ordered vector spaces. For the product space to be a Riesz space (resp. a fully lattice-ordered space), it is necessary and sufficient that each of the spaces be a Riesz space (resp. a fully lattice-ordered space).
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Let us restrict ourselves to examining the case of fully lattice-ordered spaces. Suppose that all of the are fully lattice-ordered; let be a nonempty subset of that is bounded above and let be an upper bound for . For every , is bounded above by , hence has a supremum in ; it is clear that is the supremum of in .
Conversely, suppose is fully lattice-ordered. Let be a subset of that is bounded above, the subset of formed by the such that and for . It is immediate that is bounded above in , hence has a supremum ; by the definition of the product order relation, necessarily for , and is the supremum of , which completes the proof.
Definition 3
Let be an ordered vector space, and two supplementary linear subspaces of . One says that is the ordered direct sum of and if the canonical mapping of the ordered vector space onto the ordered vector space is an isomorphism.
Proposition 4
For an ordered vector space to be the ordered direct sum of two supplementary linear subspaces , it is necessary and sufficient that the relations imply and .
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Since and imply in , the condition in the statement says that transforms the set of elements of into the set of elements of .
5. Bands in a fully lattice-ordered space
Definition 4
In a fully lattice-ordered space , a linear subspace of is said to be a band if it satisfies the following conditions: 1) the relations and imply ; 2) for every nonempty subset of that is bounded above in , the supremum of in belongs to .
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Example
In the space of real-valued functions defined on a set , the set of functions that are zero at all the points of a subset of is a band.
Remark
In the space , the subspace of bounded real-valued functions on satisfies condition 1) of Def. 4; moreover, for every subset of that is bounded above in , the upper envelope of belongs to . However, if is infinite, a subset of may be bounded above in without being bounded above in , in which case is not a band in .
It follows at once from Def. 4 that if is a band in then, for every nonempty subset of that is bounded below in , belongs to . Every band in , equipped with the ordered vector space structure induced by that of , is a fully lattice-ordered space and, for every subset that is bounded above in , the supremum of in is identical with its supremum in .
The intersection of any family of bands in a fully lattice-ordered space is also a band. For every subset , there exists a smallest band containing (since itself is a band); this band will be called the band generated by .
The properties of bands in a fully lattice-ordered space rest on the following proposition:
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Cites Definition 4
Proposition 5
— *Let be a fully lattice-ordered space, a non-empty subset of consisting of elements , such that: 1) , and 2) the relations imply . Let be the set of suprema in of those subsets of that are bounded above in . Under these conditions, every element of may be written in the form , where is the supremum of the elements such that , and where is an element that is alien to every element of .
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At any rate , so it all comes down to showing that is alien to every element (No. 1), in other words that is zero. By hypothesis, and , thus ; for every such that , by definition , thus ; since by hypothesis, also by the definition of ; finally, since is the supremum in of the elements such that and , we have , whence , which completes the proof.
Theorem 1 (F. Riesz)
— *Let be a subset of a fully lattice-ordered space . The set of elements that are alien to every element of is a band; the band of elements that are alien to every element of is identical to the band generated by , and is the ordered direct sum of the bands and .
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Cites Proposition 4, Proposition 5
Cited by Corollary, Proposition 6, Proposition 5, II § 2, V § 5. Measures defined by numerical densities, Example, V § 5, Theorem 3 (Lebesgue), V § 5
The properties of alien elements, reviewed in No. 1, and the definition of a band, show at once that is a band, hence so is . By Proposition 5 and the definition of a band, every element of may be written , with and , and being ; since every element of is the difference of two elements , we have ; on the other hand, since is the only element alien to itself, we have , which proves that is the direct sum of and ; finally, since the components in and of an element of are , is the ordered direct sum of and (No. 4, Prop. 4).
It remains to show that is identical to the band generated by . Now, is the direct sum of and the band formed by the elements alien to all the elements of ; since , we have ; on the other hand and is also the direct sum of and ; therefore necessarily , .
Theorem 1 and Proposition 5 make it possible to give another definition of the band generated by a set of elements of :
Proposition 6
— *Let be a fully lattice-ordered space, a subset of , and the band generated by . Let be the set of elements of each of which is some element of the form , where ; let be the set of suprema of those subsets of that are bounded above; then the set is identical with the set of elements of .
Clearly by the definition of a band; on the other hand, if is the band of elements that are alien to every element of , Theorem 1 shows that is the ordered direct sum of and . But Proposition 5 shows that every element of is the sum of an element of and an element of , whence the proposition.
Corollary
— *Let be an element of a fully lattice-ordered space , the band generated by , the band of elements alien to . For every element of , the component of in (for the decomposition of as the ordered direct sum of and ) is equal to .
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Cites Proposition 5, Proposition 6, Theorem 1 (F. Riesz)
Cited by Proposition 5, II § 2, Corollary 2, V § 5
This follows from Proposition 6, applied to , and Proposition 5.
Note that the bands generated by and are identical. If and are two elements of that are alien to each other, and if and are the bands generated by and , respectively, then every element of is alien to every element of ; for, belongs to the band of elements alien to , whence , and, by Theorem 1, every element of is alien to every element of .
Exercises
See the exercises for § 1.